As a generic model system of an asymmetric binary fluid mixture, hexadecanedissolved in carbon dioxide is considered, using a coarse-grained bead-springmodel for the short polymer, and a simple spherical particle with Lennard-Jonesinteractions for the carbon dioxide molecules. In previous work, it has beenshown that this model reproduces the real phase diagram reasonable well, andalso the initial stages of spinodal decomposition in the bulk following asudden expansion of the system could be studied. Using the parallelizedsimulation package ESPResSo on a multiprocessor supercomputer, phase separationof thin fluid films confined between parallel walls that are repulsive for bothtypes of molecules are simulated in a rather large system (1356 x 1356 x 67.8A^3, corresponding to about 3.2 million atoms). Following the sudden systemexpansion, a complicated interplay between phase separation in the directionsperpendicular and parallel to the walls is found: in the early stages thehexadecane molecules accumulate mostly in the center of the slit pore, but asthe coarsening of the structure in the parallel direction proceeds, theinhomogeneity in the perpendicular direction gets much reduced. Studying thenthe structure factors and correlation functions at fixed distances from thewall, the densities are essentially not conserved at these distances, and hencethe behavior differs strongly from spinodal decomposition in the bulk. Some ofthe characteristic lengths show a nonmonotonic variation with time, and simplecoarsening described by power-law growth is only observed if the domain sizesare much larger than the film thickness.
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机译:作为不对称二元流体混合物的通用模型系统,考虑了将十六烷溶解在二氧化碳中,对短聚合物使用粗粒珠弹簧模型,对二氧化碳分子使用具有Lennard-Jones相互作用的简单球形颗粒。在以前的工作中,已经表明该模型能够很好地再现真实的相图,并且还可以研究系统突增后本体中旋节线分解的初始阶段。在多处理器超级计算机上使用并行仿真软件包ESPResSo,在相当大的系统(1356 x 1356 x 67.8A ^ 3,对应于约320万个原子)中,模拟了对两种分子都排斥的平行壁之间的流体薄膜的相分离。随着系统的突然膨胀,在垂直和平行于壁的方向上发现了相分离之间的复杂相互作用:在早期阶段,十六烷分子主要聚集在狭缝孔的中心,但是随着结构在平行方向上的粗化的进行,垂直方向的不均匀性大大降低。然后研究在距壁固定距离处的结构因子和相关函数,在这些距离处密度基本上不守恒,因此,其行为与块状旋节线分解有很大不同。一些特征长度显示出随时间的非单调变化,并且仅当畴尺寸远大于薄膜厚度时,才能观察到以幂律增长描述的简单粗化。
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